the fundamentals of iv (current/voltage) measurement
TRANSCRIPT
The Fundamentals of IV (Current/Voltage)
Measurement
Alan Wadsworth Market Development Manager Americas Field Marketing
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April 10, 2012
Webcast Agenda
• IV Measurement Basics • Source/Measure Units (SMU) Introduction • Low Current Measurement Techniques • Making Accurate Resistance Measurements • B2900A SMU Series Features & Benefits • Final Remarks
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IV MEASUREMENT BASICS
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What is Current?
Page 4
Negative charge (electrons) flowing in the negative x direction is equivalent to positive charge flowing in the positive x direction.
Note: In semiconductors it is possible to measure the flow of positively charged electron holes.
- - + -
x
- - -
- - -
- -
Understanding Accuracy & Repeatability
High accuracy, low repeatability Low accuracy, high repeatability
Accuracy – The degree of conformity of a measured or calculated quantity to its actual (true) value. Repeatability (aka precision) – The degree to which repeated measurements or calculations show the same or similar results.
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Understanding Measurement Resolution
Simplified analog-to-digital converter (ADC) circuit.
Resolution – The smallest change in data that an instrument can display.
The number of bits available to the digital-to-analog converter (DAC) determines the fineness of the measurement detail.
Example: 20 bits of resolution represents the ability to distinguish one part in 220 or 1,048,576.
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What is a Half Digit of Resolution?
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Be careful! This can mean different things for different instruments
Question: What is the ½ digit here?
Answer: It is the 7. In this case the least significant digit only has ½ the resolution of the other digits.
Why Are Triaxial Cables Needed for Low-Current?
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BNC (Coaxial) Cable: Triaxial Cable:
Leakage Current: Leakage Current:
Triaxial cable reduces leakage current by a factor of 100,000,000.
What is a 4-Wire (Kelvin) Measurement?
Rcable
Rcable
Rcable
Rcable
IForce
+ - VSense
I=0 I=0
Force Line 1 Force Line 2
Sense Line 1 Sense Line 2
RDUT
Eliminate cable resistance from the measurement
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Example Instrument Outputs (Banana Jack)
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Sense Force Guard High
Low
± 250V = Max
± 210V = Max
By default the low outputs are tied to chassis ground, but in this case they can be floated up to 250 V above or below chassis ground if desired.
This tells you the maximum allowable voltage (210 V in this case) between the high and low inputs.
When making a basic 2-wire measurement you should use the Force outputs.
4-wire measurements require the use of the Sense lines in addition to the Force lines.
SOURCE/MEASURE UNIT (SMU) INTRODUCTION
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What is a Source/Measure Unit (SMU)?
Note: The tight integration of these measurement resources yields better accuracy and faster measurement than would an equivalent collection of separate instruments.
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Simplified equivalent circuit (2-wire measurements):
Ideal Voltage Source
Ideal Current Source
Ammeter
Voltmeter Chassis Ground
A
V
+ -
+
-
High Force
Low Force
+ -
Why Would You Use an SMU for IV Measurements?
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VFIM (Force voltage & measure current)
IFVM (Force current & measure voltage)
ADUT DUTV
An SMU integrates the following capabilities into each channel: • Four-quadrant voltage source • Four-quadrant current source • Voltage meter • Current meter
Here are the two most common modes of operation:
Why Use a Benchtop SMU for IV Measurements? Reason #1: Improved Measurement Efficiency
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Multimeter
Multimeter
DC Voltage Source
DC Voltage Source
DUT
RL
Bench-top setup example for 4-terminal DUT
IN OUT DUTIN OUT
B2900A setup example for 4-terminal DUT
Channel 2 on the back side
Channel 1
Problem: Limited bench-top space for single-function instruments. Solution: A benchtop SMU reduces the number of instruments and reduces
messy wiring.
Non-SMU setup example for 4-terminal device
SMU setup example for 4-terminal device
Why Use a Benchtop SMU for IV Measurements? Reason #2: Eliminate the Need for a PC
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Problem: Many bench-top instruments require a PC to graphically display data and to make measurements.
Solution: A GUI-based benchtop SMU supports real-time IV curve monitoring directly on the instrument. You can also save graphs and data to a flash drive for report generation.
Dump toUSB memoryMeasurementSet SMUs for DUT
Quick Evaluation
Report
Organize your quick report
LOW CURRENT MEASUREMENT TECHNIQUES
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Low-Current Measurement Challenges
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???
• How do I eliminate electromagnetic interference?
• How do I avoid creating ground loops?
• What is measurement ranging and how do I optimize it?
• Why is integration time important in eliminating noise?
• How do I eliminate voltage and current transients?
Use Shielding to Avoid Electromagnetic Interference
Shielding Box
Probing Equipment and DUT
Note: Shielding is not the same as guarding.
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Avoiding Ground Loops
Conductive planes tied together at only one point cannot have any current flowing between them.
Conductive planes tied together at multiple points creates a loop for current (a condition to be avoided).
Do not connect up equipment to ground at more than one point!
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Understanding Measurement Ranging - 1
All measurement circuitry needs to switch in and out various resistors in order to measure currents and voltages at different levels. The measurement range determines the maximum measurement resolution that you can obtain*.
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*Typically 5 decades below the measurement range.
Understanding Measurement Ranging - 2
10 pA
100 pA
1 nA
10 mA
100 mA
Fixed Ranging – Always stay in the same measurement range
Limited Ranging – Never go below the specified range limit
Auto Ranging – Go as low as necessary to make an accurate measurement (down to the lowest range supported if necessary)
Current Measurement Range
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Integration Time Eliminates Measurement Noise AC Voltage
Time
Time
Measured Value Averaged over multiple power line cycles
Integration DOES NOT have any effect on the measurement resolution.
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Eliminating Transient Effects
Delay Time
SMU Output
Time
Hold Time
Measurement
The hold time and delay time settings allow you to specify how long to wait before starting a measurement after the SMU applies voltage or current.
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Step #1: Perform Self-calibration
Before performing Self Calibration After performing Self Calibration
1 nA
1 fA
1 pA 100 fA
Almost all instruments designed for low-current measurement have some sort of self-calibration mechanism. It is important that you DO THIS before attempting a low-current measurement. Note: B2900A example shown
Press the System > Cal/Test function keys
From the front panel:
Press OK to perform Self-calibration
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Step #2: Select the Correct Current Measurement Range
Using 1 µA Current Measurement Range: Using 10 nA Current Measurement Range:
1 nA
1 fA
10 pA 100 fA
From the front panel: In Single View mode you can specify the current measurement range.
Most instruments DO NOT boot up in their lowest measurement range. In this example notice the improvement in measurement performance obtained by changing from the 1 µA current measurement range to the 10 nA current measurement range. Note: B2900A example shown
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Step #3: Increase the Integration Time to Eliminate Measurement Noise
Using SHORT(0.01 PLC) integration time: Using NORMAL (1 PLC) integration time:
1 nA
1 fA
1 pA 100 fA
From the front panel: In Single View mode you can select the measure-ment speed (integration time)
In general, low-current measurements need at least 1 power line cycle (PLC) of integration to obtain decent results (in this example NORMAL integration). Extremely low currents and/or noisy environments may require LONG integration (16 PLCs). You can use MANUAL integration to select PLC values between these two extremes. Note: B2900A example shown
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Step #4: Select an Appropriate Measurement Trigger Delay Time
Using a Trigger Delay Time of 0 ms Using a Trigger Delay Time of 200 ms
1 nA
1 fA
5 pA 100 fA
From the front panel: In Single View mode you can select the measure-ment delay time
The length of the wait time depends primarily on the size of the voltage step; larger voltage steps require longer wait times. However, the magnitude of the capacitance being driven also impacts the wait time (larger C longer wait times). Note: B2900A example shown
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Important! Current Measurements <1 nA Require Triaxial Cabling & Fixturing
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Kelvin Adapter Non-Kelvin Adapter
N1294A-001 Banana–Triaxial Adapter for 2-wire connection (non-Kelvin) N1294A-002 Banana–Triaxial Adapter for 4-wire connection (Kelvin)
MAKING ACCURATE RESISTANCE MEASUREMENTS
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L
W
d LWdR
LAR ==ρ
+
-
IVR = V
I
Page 30
Understanding Resistivity and Resistance
When characterizing materials we typically want to know the resistivity, which is a material property that is independent of the dimensions of the device being measured.
=
)||()||( SSSSS RRRRR +=
Rs Rs
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Understanding “Ohms per Square”
You may sometimes see the term “Ohms per Square”. This is simply another way of specifying resistivity. As long as the thickness of a material is constant, it has the same measured resistance for any sized square of the material.
Measuring Resistance: A Trivial Measurement?
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V = I x R, correct? NO!
V = I x R(T) Resistance depends on temperature!
Resistance measurement is a tricky balance between two factors:
1. To keep the resistor from heating up and the resistance value from changing, we need to keep the current (= power) low.
2. Small currents imply that we need to measure smaller voltages, which in-turn requires more voltage measurement resolution capability.
This is referred to as the Joule self-heating effect.
SiO2
1 cm 0.014 W/oC-cm2
(h × 71) oC-cm2/W, or 0.007 oC-cm2/W for h = 1 µm
SiO2
1 cm
h
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The Importance of Thermal Resistance
• For a 1 cm2 block of SiO2 1 µm thick, if you apply 1 W the temperature will rise by 0.007 oC
• For a 10 µm2 block of SiO2 1 µm thick, if you apply 1 W the temperature will rise by 7,000 oC!
How Much Power Can I Apply to a Structure?
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RV
RVVIVP
2
=×=×= )(maxmax TRPV ×=
At or near room temperature the resistance of a Cu or Al metal line changes by about 0.35%/oC. This allows us to compute the maximum amount of power that can be dissipated to produce a 0.1% change in resistance for a Cu or Al metal square 10 mm by 10 mm.
mWPcmmmmmCWcmCP oo
04.0)1/10()10/(1/%35.0/007.0%1.0
max
222max
=∴×××−×=
To achieve 0.1% accuracy in a copper structure with an equivalent resistance of 10 mΩ per square (1 mm thick film) we have the following:
VmmWV 000632.0)10()04.0(max ≈Ω×=
Need 1 µV of voltage measurement resolution!
Thermo Electro-Motive Force (EMF): What is It?
EMF: A transient voltage pulse that is associated with reed relay switches.
Thermo-EMF example of general reed relay
-1.E-05
0.E+00
1.E-05
2.E-05
3.E-05
0 500 1000 1500 2000Time (s)
Vm
(V)
Note: This is NOT an example of the relays used in our instrumentation.
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EMF can have a significant impact on low-level resistance measurements.
Modified Kelvin Resistance Measurement Key Points: 1) Make sure that you eliminate Joule
self-heating effects 2) Measure twice and average the two
resistances
VMU 2 (SMU 4)
SMU 2
VMU 1 (SMU 3)
SMU 1
R Force Current Twice (both ways), i.e. +/- IF
VM1 V
0 V
VMU 1 (SMU 3)
VM1
VEMF1
VOFF1 + - + -
VMU 2 (SMU 4)
VM2
VEMF2
VOFF2 + - + -
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B2900A SMU SERIES FEATURES & BENEFITS
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B2900A Series of Precision Source/Measure Units
B2900A Key Features: 1. Range of up to ±210 V and ±3 A (DC) / ±10.5 A (pulsed)
provides wider coverage for testing a variety of devices
2. Measurement resolution of 10 fA and 100 nV offers better source and measurement performance
3. GUI for quick bench-top testing, debug and characterization
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Interactive Device Evaluation Can be Performed Entirely from the Front Panel (4 Viewing Modes):
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Dual Channel View (2-ch Units Only) Single Channel View
Graph View (I-V, I-t, and V-t plots) Roll View (similar to strip chart)
Setting Up a Sweep Measurement from the Front Panel is Easy!
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Speed
Show Sweep
Show Pulse
Show Trigger
More…
Assist Keys Sweep Settings Sweep Type
B2900A Series Sourcing Capabilities
Constant Linear Sweep Single Double
Log Sweep Single Double
List Sweep
DC
Pulse
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
V or I
t
Source Function
V or I
t
V or I
t
Arbitrary Waveform Generation The List Sweep function allows you to create arbitrary waveforms with up to 2500 steps. The timing resolution varies by B2900A model (20µs for B2901/02A, 10µs for B2911/12A ).
An icon appears in the GUI to indicate the type of sweep function selected.
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B2900A Series Measurement Capabilities
High Speed Digitizing Capability In addition to its intrinsic measurement functions, the B2900A Series has an advanced trigger design that enables high speed digitizing measurements (20µs for B2901/02A, 10µs for B2911/12A).
V or I
t 20µs for B2901/02A 10µs for B2911/12A
:Measurement
The B2900A Series has four measurement functions that can be selected for either channel using its front-panel GUI or SCPI commands.
Voltage Measurement Current Measurement Resistance Measurement Power Measurement
Note: The Power Measurement function cannot be specified when using remote control
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B2900A Maximum Voltage and Current Output
Maximum Voltage Maximum Current
DC or Pulsed
210 V 0.105 A
21 V 1.515 A2
6 V 3.03 A2
Pulsed only1
200 V 1.515 A
6 V 10.5 A
1. Maximum duty cycle is 2.5% 2. On 2-channel units some additional restrictions apply on the combined current
output of both channels (please refer to data sheet)
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The B2900A Allows You to View Graphical Measurement Results
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Roll View Provides a Convenient Way to View Slow-Moving Voltages/Currents Over Time
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Can capture low-frequency “glitches”.
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Agilent Has Free “Quick I/V” Software for Customers Wanting PC-Based Instrument Control
B2900A Series Model Comparison
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Model # of SMUCh’s
Set/Measure Range Setting Resolution Measurement
Resolution Digitizing
Rate (sample/s)
Other Features Approximate
Pricing (US) Digits
Min. Resolution Digits
Min. Resolution
V I I V I V
B2901A 1
±210V
±3A/ch (DC) ±10.5A/ch (Pulsed)
5½ 1pA 1μV 6½ 100fA 100nV 50 k/sec (20µs/pt)
• XY View • AWG/List Sweep
$5.8K
B2902A 2 $8.5K
B2911A 1 6½ 10fA 100nV 6½ 10fA 100nV 100 k/sec
(10µs/pt)
• XY View • AWG/List Sweep • Roll View
$8.3K
B2912A 2 $12.8K
FINAL REMARKS
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Additional Agilent SMU Instrument Products
Year 80 85 90 95 00 05 10
HP 4142B
4155/56 series 4145 series
E5260A/70B series
Modular SMU
Parameter Analyzer
Bench-top SMUs B2900A series
B1500A/B1505A
Agilent has more then 30 years of instrument SMU experience.
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Device Analyzer
USB SMU
U2722A/23A N678xA SMU
Power Analyzer
Comparison of the B1500A & B1505A
Software EasyEXPERT
– Tracer Test – Classic Test – Application Test – Quick Test
Modules MPSMU HRSMU ASU HV-SPGU WGFMU
Modules HCSMU HVSMU
Accessories SCUU GSWU
Accessories HV Bias-T Module Selector Unit
Max I/V - 1 A, 200 V Meas. Res. - 0.1 fA, 0.5 µV
Modules HPSMU MFCMU
B1500A B1505A
Max I/V - 40 A, 3000 V Meas. Res. - 10 fA, 2 µV
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Parametric Measurement Handbook Available
You can download the PDF file (Rev 3) from the web: http://www.agilent.com/find/parametrichandbook You can also request it after completing the evaluation form.
>200 pages of invaluable information on parametric test
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Question & Answer Session
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